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Velocity of sound in a medium is given b...

Velocity of sound in a medium is given by `A^(1//2) d^(-1//2)`, where 'd' is density of medium. Then A represents

A

Elastic constant

B

Energy

C

Volume

D

Compressibility

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To solve the problem, we need to analyze the given equation for the velocity of sound in a medium, which is expressed as: \[ v = A^{1/2} d^{-1/2} \] where \( v \) is the velocity of sound and \( d \) is the density of the medium. Our goal is to determine what \( A \) represents. ### Step 1: Rearranging the equation We start by squaring both sides of the equation to eliminate the square root: \[ v^2 = A \cdot d^{-1} \] This can be rewritten as: \[ v^2 = \frac{A}{d} \] ### Step 2: Isolating \( A \) Next, we can isolate \( A \) by multiplying both sides by \( d \): \[ A = v^2 \cdot d \] ### Step 3: Finding the dimensions of \( A \) Now, we need to express \( A \) in terms of its dimensional formula. We know the dimensions of \( v \) (velocity) and \( d \) (density): - The dimension of velocity \( v \) is given by: \[ [v] = L T^{-1} \] - The dimension of density \( d \) is given by: \[ [d] = M L^{-3} \] ### Step 4: Calculating the dimensions of \( A \) Substituting the dimensions of \( v \) and \( d \) into the equation for \( A \): \[ A = (L T^{-1})^2 \cdot (M L^{-3}) \] Calculating this gives: \[ A = L^2 T^{-2} \cdot M L^{-3} \] Now, we can combine the dimensions: \[ A = M L^{2 - 3} T^{-2} = M L^{-1} T^{-2} \] ### Step 5: Identifying what \( A \) represents The dimensional formula \( M L^{-1} T^{-2} \) corresponds to the dimensional formula for the elastic constant (also known as the modulus of elasticity), which is defined as stress (force per unit area) divided by strain (dimensionless). ### Conclusion Thus, we conclude that \( A \) represents the elastic constant of the medium.
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